Double-Buck PFC Converter
发布时间:2024-11-02
发布时间:2024-11-02
6660IEEETRANSACTIONSONPOWERELECTRONICS,VOL.29,NO.12,DECEMBER2014
DesignandImplementationofaTransformerlessSingle-StageSingle-SwitchDouble-BuckConverterWithLowDC-linkVoltage,HighStep-Down,andConstantInputPowerFactorFeatures
YuChen,Member,IEEE,ZhihaoZhong,andYongKang
Abstract—Thispaperpresentsanewtransformerlesssingle-stagesingle-switch(S4)converterwhichintegratesabuck-typepowerfactorcorrectioncellwithabuck-typedc–dcoutputcellinaspecialway.TheproposedconverterpreservestheadvantagesofexistingtransformerlessS4converters,suchasthelowvoltagestressacrossthedc-linkcapacitor,lowcurrentstressoftheswitch,andhighstep-downinput-to-outputvoltage.Moreover,thepro-posedconverterprovidesanewattractivefeature,i.e.,itsinputpowerfactoralwayskeepsconstantevenwhentheline-andload-conditionsvary.Thesecharacteristicsmaketheproposedconvertercost-ef cient,easy-to-design,andsuitableforthelow-powerandnonisolatedapplications.Theprincipleandanalysisofthepro-posedconverterarepresentedinthispaper,andadesignexampleisalsogiventoshowthevalidityofanalysis.
IndexTerms—LEDdriver,powerelectronics,powerfactorcorrection(PFC),single-stagesingle-switch(S4)converter.
I.INTRODUCTION
M
ANYindustrialapplicationsrequirenotonlyatightdcvoltagetofeedtheirloads,butalsoahigh-inputpower
factor(PF)toreduceharmonicdistortioninthecurrentdrawnfromthegrid.Theserequirementscanbesimplysatis edbyasinglepowerfactorcorrection(PFC)converter[1]–[8].How-ever,itsoutputvoltagehasthehighripplesattwiceofthelinefrequency.Theseripplesgetevenhigherwhentheoutputvoltagebecomeslowerandtheloadbecomesheavier.TheothersolutionisusingaPFCconverterincascadewithadc–dcconverter,withwhichtheinstantaneousinputpowerandthestableoutputpowercanbedecoupledbyanintermediatedc-linkcapacitor[9]–[13].However,suchatwo-stagecon gurationsuffersfromthein-creasedcomponentcount,highcost,andcomplicatedcontrol.
ManuscriptreceivedAugust17,2013;revisedNovember3,2013andJanuary8,2014;acceptedFebruary5,2014.DateofpublicationFebruary14,2014;dateofcurrentversionAugust13,2014.ThisworkwassupportedbytheLite-OnPowerElectronicsTechnologyResearchFundunderGrant2012-04andSpe-cializedResearchFundfortheDoctoralProgramofHigherEducationunderGrant20120142120026.ThispaperwaspresentedinpartattheIEEEEnergyConversionCongressandExposition,2013.RecommendedforpublicationbyAssociateEditorT.Qian.
TheauthorsarewiththeStateKeyLaboratoryofAdvancedElectromagneticEngineeringandTechnologyandtheSchoolofElectricalandElectronicEn-gineering,HuazhongUniversityofScienceandTechnology,Wuhan430074,China(e-mail:ayu03@http://;cobeam@http://;ykang@http://).Colorversionsofoneormoreofthe guresinthispaperareavailableonlineathttp://.
DigitalObjectIdenti er10.1109/TPEL.2014.2306430
Tocompromisethesize,cost,andperformance,manysingle-stagesingle-switch(S4)convertershavebeenproposed.Fromthetopologypointofview,S4converterscanbetreatedasanintegrationversionofthetwo-stagestructure,inwhichtheswitchesinthePFCanddc–dcconverterarecombinedasone.Severaladvantagescanbeobtainedusingthisintegrationapproach:1)thePFCanddc–dccellsshareoneswitch,thesizeandcostcanbereduced;2)thehighinputPFcanbeobtainedautomaticallybythePFCcellwiththediscontinuousconductionmode(DCM),onlytheoutputvoltageneedstoberegulated,thecontrollercanbesimple;and3)theinputandoutputpowercanstillbedecoupledsincetheintermediatedc-linkcapacitorisremained,thereforethevoltageripplesintheoutputarealleviated.Duetothesefeatures,S4convertersareespeciallysuitableforthelow-powerapplicationswithcriticalsizeandcostlimitations.
S4converterswithgalvanicisolationhavebeenwellstud-iedinthepastdecades[14]–[29].However,insomelightingapplications,galvanicisolationisnotmandatorybythesafetyrequirementsorstandards.Forexample,thedriverforemergingsolid-statelightingcouldbenonisolated,astheexistingincan-descentlampsarealsonotisolatedfromthegrid[2],[30]–[32].Insuchacase,transformerlessS4convertersaremorecom-pactandcost-ef cientsolutions.Unfortunately,ifalowoutputvoltageisneeded,anextremelynarrowdutycycleisrequiredinsuchkindofconverterswithoututilizingatransformer,es-peciallyinthehigh-linecondition.Thenarrowdutycycleishardtoberealizedbyalow-costPWMcontrollerandleadstoapooref ciency[3],[33],[34].Therefore,thetopologydesignforsuchtransformerlessS4convertersshouldcompromisenotonlyagoodinputPFandastableoutputvoltage,butalsoahigh-voltagestep-downfeature(i.e.,alowoutputvoltagebutarelativelylargedutycycle).
Recently,severaltransformerlessS4convertershavebeenpresentedtomeettheaforementionedrequirements.Theboost/buck-boostS4converterispresentedin[35].TheboostPFCcellprovidesagoodinputPF,butitalsorequiresahighdc-linkvoltage,whichdegradestheconverter’sstep-downfeature.TheS4converterswithbuck-boostPFCcells[33],[34],[36]reducethedc-linkvoltage,andthevoltagestep-downcanberealizedbyabuck[34],quadraticbuck[33],orbuck-boost[36]cell.However,thesingleswitchintheaforementionedconvert-ersneedstohandlethecurrentsofbothcells,whichleadstothethermalproblemoftheswitch.In[37]and[38],abuck/
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Fig.1.
ProposedtransformerlessS4converter.
buck-boostS4converterisproposedtofurtherreducethedc-linkvoltageandenhancethestep-downfeature,andthesingle-switchdoesnotneedtohandlethecurrentsofbothcells.How-ever,sinceitsPFCcellisbucktype,thecircuitmustbecarefullydesignedsothatasatisfactoryinputPFcanbeobtainedinthecaseoftheline-andload-conditionsvariation.
Toovercomethedrawbacksoftheaforementionedtrans-formerlessS4converterbutpreservetheiradvantages,thispaperproposesanewtopologythatintegratesabuckPFCandbuckdc–dccells,asshowninFig.1.Abuckdc–dccellisembeddedinthecircuit(thecomponentshighlightedinblue),wherethedc-linkcapacitorCbistreatedasitsinput;ontheotherhand,ifSisturnedONandDakeepsconducting(theconductionofDawillbeguaranteedbytheparameterdesign,asdiscussedlater),nodeaandnodebwouldhavethesamevoltagepotential,thecomponentsinredconstructanequivalentbuckPFCcell,inwhichvinistreatedasinput,CbinserieswithCoistreatedasoutput.Withsuchintegration,thefollowingbene tscanbeobtained:
1)theequivalentbuckPFCleadstoalowvoltagestressacrossthedc-linkcapacitorCb,theelectrolyticcapacitorswithlowvoltageratingbutlargecapacitycanbeused;2)thesingleswitchSneedstohandleonlythecurrentofthedc–dccell,thecurrentstressislow;
3)integrationoftwobuckcellsleadstothehighstep-downinput-to-outputvoltage;
4)fortheequivalentbuckPFCcell,itsequivalentsink,Cb
andCo,inserieswiththereversedpolarities.Thisstruc-turebringsinanattractiveconstantPFfeature,whichisindependentoftheline-andload-conditions.Thisuniquefeaturefacilitatesthecircuitdesignalot.
Toclearlyexplaintheaforementionedcharacteristics,theop-erationalmodesoftheproposedS4converterarepresentedinSectionII.Then,thecircuitcharacteristicsareanalyzedinSec-tionIII.Accordingtotheanalysis,aneasy-to-followdesignprocedure,adesignexample,anditsexperimentalresultsaregiveninSectionIV.Theconclusionsare nallygiveninSectionV.
II.OPERATIONALMODESOFTHEPROPOSEDS4CONVERTERA.De nitionsofRegionIandRegionII
Tosimplifytheanalysis,allcomponentsaretreatedasideal;thedclinkandoutputcapacitorsarelargeenough,thereforetheirvoltageVbandVoaretreatedasconstantwithinhalf
of
Fig.2.
TwoworkingregionsoftheproposedS4
converter.
Fig.3.KeywaveformsoftheproposedS4converter:(a)inregionIand(b)inregionII.
line-cycleperiod;andaftertherecti er,theinputvoltagevinhasbeenrecti edasvg(θ)=|vin|=|Vpksinθ|,whereVpkisthepeakvoltageofvin,andθisavariablevaluefrom0to2π.Especially,consideringhalfofline-cyclefrom0toπ,vg(θ)canbeexpressedas
vg(θ)=|vin|=Vpksinθ
θ∈[0,π].
(1a)
TheproposedS4converterincludesabuck-typePFCcell,therefore,twoworkingregionscanbefoundwithinhalfofline-cycleperiod,asshowninFig.2.Withtheproposedintegration,theequivalentvoltageVeq=Vb VoactsasthesinkofthePFCcell,therecti erdoesnotconductwhenvg(θ)<Veq,thisintervalisde nedasRegionI.Oppositely,ifvg(θ)>Veq,therecti erconductsandainputcurrentiinappears.Thisintervalisde nedasRegionII.ThestartpointαandendpointβofRegionIIhavebeenmarkedinFig.2,theycanbeexpressedas
α=arcsin
Veq
Vandβ=π arcsinVeq.pkV(1b)
pk
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Basedonthesede nitions,thekeywaveformsineachregionaregiveninFig.3,andtheoperationalmodesareshowninFig.4,theyareanalyzedasfollows.B.OperationalModesinRegionI
M1(t0 t1):SwitchSisturnedON,thevoltageappliedonL2isVeq=Vb Vo,iL2increaseslinearlyfromzerowiththeslopeVeq/L2;ontheotherhand,thevoltageappliedontherecti erdiodesisvg(θ) Veq.Noticingvg(θ)<Veqinthisre-gion,therecti erisblocked,thereisnocurrent owingthroughL1,iL1=iin=0.ThismodewillpersistuntilSisturnedOFFatt1.Denotingtheduty-cycleasd,thepeakvalueofiL2att1canbecalculatedas
IVL2 pk=eq
LdT2s.(2a)
SinceiL2also owsthroughSandCb,thepeakvaluesofiCbandiSarealsoIL2 pk.
M2(t1 t2):SisturnedOFF,iL2isfreewheelingthroughD2,iL2decreaseslinearlywiththeslopeVo/L2.Thecurrent owingthroughCbandSisnowzero;inthePFCcell,iL1andiinarealsozero,whichisthesameasM1.ThismodewillpersistuntiliL2decreasestozeroatt2.DenotingthedutycycleinthismodeasdDC,itcanbesolvedas
dDC=
Veq
Vd.(2b)
o
M3(t2 t3):OnceiL2decreasestozero,itkeepszerountil
SisturnedONagain.Inthismode,onlytheenergyinCoisreleasedtoRo,thecurrents owingthroughL1,L2,Cb,andSareallzero.
AccordingtotheoperationalmodesinRegionI,theequiv-alentcircuitofthedc–dccellisalsoshowninM1–M3(seeFig.4).Obviously,thedc–dccellisactuallyabuckconverterworkingintheDCM;whilethePFCcellisdeactivatedduringthisregion.
C.OperationalModesinRegionII
M4(t0 t1):WhenSisturnedONinthiscase,thevoltageacrossL2isVeq=Vb Vo,whichisthesameasthatinM1.AndsinceDaalsoconducts,nodesaandbhavethesamevoltagelevels,itmeansthevoltageappliedonL1isvg(θ) Veq.Noticingvg(θ)>Veq,therecti erisconductedandiL1beginstoincreaselinearlyfromzerowiththeslope[vg(θ) Veq]/L1.Itshouldbeemphasizedthat,thismodeispersistingonlywhenDaisconducting.ItmeansiS>iin,orequivalentlyiL2>iL1mustbesatis ed,sothatthedifferencecurrentiDacanbeextractedfromCbthroughDa,andthus,keepsDaconducting.Thisrestrictionissatis edbytheappropriateparameterdesigninSectionIII.Thismodewillpersistuntilt1whenSisturnedOFF.Att1,thepeakcurrentIL2 pkandIS pkarethesameas(2a),andthepeakvalueofiL1andiincanbecalculatedas
IL1 pk=I=v(θ) Vin pk
geqLdTs.
(2c)
1
M5(t1 t2):SisturnedOFF.Inthedc–dccell,iL2isfree-wheelingthroughD2,thevoltageappliedonL2is Vo,there-
foreiL2decreaseslinearlywiththeslope Vo/L2,and nallyreacheszeroatt2.ThecorrespondingdutycycledDCisthesameasthatin(2b).InthePFCcell,iL1isfreewheelingthroughD1,thevoltageappliedonLV1is Veq,iL1decreaseswiththeslope eq/L1.Inthismode,iinkeepszeroandiCbalwaysequalsto iL1.
M6(t2 t3):iL2hasdecreasedtozero,iL1keepsdecreasingbecausethevoltageappliedonL1isstillVeq.iL1will nallyreachzeroatt3.ThecorrespondingdutycycledPFCcanbesolvedas
dv VPFC=
g(θ)eq
Vd.
(2d)
eq
M3(t3 t4):BothiL1andiL2arezero,thecircuitstategoestoM3,asthatinregionI.
TheequivalentcircuitsofthePFCanddc–dccellsinRegionIIarealsodrawninM3–M6(seeFig.4).Itisseenthatthedc–dccellstillworksasabuckconverter,andtheequivalentPFCcellalsobehavesasabuckPFC,whereL1isthebuck-inductor,Veq=Vb Voistheequivalentoutput,andD1isthefreewheel-ingdiode.Itshouldbeemphasizedthat,ifiL1decreasestozero rst,theorderofM5andM6shouldbeexchanged;how-ever,theexpressionsofdDCanddPFCarenotchangedbecausethetwofreewheelingcurrentsarecompletelyindependent.Thispossibilitywillnotberepeatedlydiscussedhere.
III.CIRCUITANALYSIS
Withtheproposedintegration,Veq=Vb VoistreatedastheequivalentsinkofthePFCcell.Tofacilitatetheanalysis,thepeak-input-to-equivalent-sinkratioMpeandtheinductionratioLare rstde nedasfollows:
MVpe=
eqVandL=L2
.(3)
pkL1
Basedonthede nitions,thecircuitcharacteristicsthatareindependentanddependentontheline-andload-conditionsareanalyzed,respectively.
A.Line-andLoad-IndependentCharacteristics
1)Single-ValuedRelationBetweenLandMpe:IneitherRegionIorII,iCb,thecurrents owingthroughthedc-linkcapacitorCbwithinoneswitchingperiodaretriangle-form,theiraveragevaluescanbecalculatedas
iCb I 1
Ts=2dIL2 pkand iCb II Ts
=12d(I1
L2 pk IL1 pk) 2
dPFCIL1 pk.(4a)Inthesteadystate,theaveragecurrent owingthroughCb
withinhalfofline-cycleperiodshouldbezero
α
β
2
b ICb II0 iC Tsdθ+
α
i Tsdθ=0.
(4b)
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Fig.4.OperationalmodesoftheproposedS4converter.
BasedontheanalysisinSectionII,(4b)canbe nallycalcu-latedas
L=
2
2πMpe
followingrestriction:
IL2 pk>IL1 pk.
as
2πMpe(1 Mpe)
<1.
2π 2arcsinMpe 2·Mpe1 Mpe
(5b)(5a)
π 2arcsinMpe 2·Mpe
21 Mpe
.(4c)
Using(2a),(2c),and(4c),(5a)canbeequivalentlyexpressed
SinceMpe>0,Lisasingle-valuedfunctionthatonlyrelatesto
Mpe.NoticingthatLisactuallyacircuitparameterdeterminedbythedesigner,theconclusion(4c)exposesthatthecircuitstateMpebecomesconstantonceLischosen,regardlessoftheline-andload-conditionsvariation.
2)CircuitRestrictionforDaConduction:ToensurethatDaisconducting,theconditioniL2>iL1mustbesatis edduringM4.SinceiL1andiL2increasefromzerototheirpeakvaluesIL1 pkandIL2 pk,respectively,iL2>iL1isequivalenttothe
De ningtheexpressionontheleftsidein(5b)asFDa,theMpeversusFDacurvecanbecalculatedasshowninFig.5(a).ItisseenthatifMpe<0.416,FDawillbesmallerthan1andthus,thecondition(5b)willalwaysbesatis ed.Ontheotherhand,therelationbetweenLandMpein(4c)canbedrawnasshowninFig.5(b).SubstitutingMpe=0.416into(4c),theequivalentrestrictionL<0.712canalsobeobtained.
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Fig.5.Line-andload-independentcharacteristics(a)MpeversusFDa,(b)MpeversusL,(c)Mpeversusγ,and(d)MpeversusPF.
3)LengthofRegionIIandtheInputPF:γ,thelengthofregionII(seeFig.2)canbeexpressedas
γ=π 2α=π 2arcsinMpe.
(6a)
Obviously,γisalsoasingle-valuedfunctionthatonlyrelatestoMpebutindependentoftheline-andload-conditions.TheMpeversusγcurveisshowninFig.5(c).ItisseenthatthesmallerMpeleadstothehigherγ,andthus,themoresinusoidal-likeaverageinputcurrent.Also,itiswellknownthatγisdirectlylinkedtotheinputPFinthebuckPFC;thus,itcanbeexpectedthattheinputPFisalsoasingle-valuedfunctionofMpe.Toprovethis,theaverageinputcurrentwithinoneswitchperiodinregionIIiscalculatedas
iin II Ts=
1
dIL1 pk.2
(6b)
ThecalculationshowsthatthePFisalsoasingle-valuedfunctionofMpe.TheMpeversusPFcurveisdrawninFig.5(d).ItisseenthatthelargerMperesultsinthelowerinputPF.However,evenMpeischosenasitsmaximalvalue0.416(tosatisfytherestrictionforDaconduction),PF=0.961isstillhighenough[38].
B.Line-andLoad-DependentCharacteristics
TheaforementionedpartpresentsthecircuitcharacteristicsthatonlyrelatetoMpe(ortheinductionratioL);however,othervariablessuchasthedc-linkvoltage,duty-cycle,voltage,andcurrentstressesofthedevicesaredependentnotonlyonMpe,butalsoontheline-andload-conditions.Theseissuesarediscussedinthispart.
1)DC-LinkVoltageVb:NoticingVeq=Vb Vo,thedc-linkvoltageVbcanbeexpressedas
Vb=MpeVpk+Vo.
(7)
Inhalfoftheline-cycleperiod,theaverageinputpowerandthermsinputcurrentarecalculatedas
1β
Pin=Vpksin(θ)· iin II Tsdθand
πα
1β
Iinrms=( iin II Ts)2dθ.(6c)
παAccordingtothede nitionoftheinputPF,thefollowingexpressioncanbeobtained:
√γ 2Mpe1 M2pe2Pin
PF== . VpkIinrms
πγ1+2M21 M2pe 6πMpepe
(6d)
ItisseenthatVbisproportionaltotheinputvoltageVpk
withthescaledcoef cientMpeandshiftedbyadcbiasVo.EvenVpkandVohavebeendetermined,asatisfactoryVbcanstillbeobtainedbychoosingaproperMpe.ToillustratethevariationofVb,(7)canbecalculatednumericallyasFig.6(a).InFig.6(a),thex-axisdenotesthevariationofVpkfrom127to373V(correspondingtothermsinputvoltagefrom90to264V);they-axisdenotesthevariationofVofrom5to48V,whichmeetsmostrequirements;andthez-axisdenotesthevalueofVbunderacertainoperationalpoint(Vpk,Vo).ItisseenthatifMpeischosenas0.22or0.31(i.e.,PF=0.99orPF=0.98),Vb<160Vcanberealizedinmostoftheoperationalpoints,anelectrolyticcapacitorwith160Vratingvoltagethuscanbe
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Fig.6.Line-andload-dependentcharacteristics:(a)dc-linkvoltageand(b)DCMrestriction.
used;andifMpeisselectedas0.37or0.41(i.e.,PF=0.97or0.96),Vb>160VmayhappenwhenthecircuitgoesintocertainoperationalregionwherebothVpkandVoarehigh.2)DCMRestriction:Fig.6(a)showsthatalowdc-linkvolt-agecanbeobtainedbyselectingasmallMpe,atthesametimeahigherinputPFcanalsobeobtained;however,theavailableminimalMpeislimitedbytheDCMcondition.Firstofall,toensuretheDCMinbothPFCanddc–dccells,iL1andiL2mustdecreasetozerowithinoneswitchingperiod.Thefollowingrelationsthusshouldbesatis ed:
d+dDC<1andd+dPFC<1.
(8a)
Substituting(2b)and(2d)into(8a),therestrictionscanbeexpressedas
d<
Vo
VVandd<M(8b)
o+Mpepk
pe.
And,sinceboththePFCanddc–dccellsneedtobemain-tainedintheDCM,thetworestrictionsmustbesatis edsyn-
chronously.Theminimalvalueofthemmustbeselectedastheboundaryrestriction
dVDCM=min
o
VM,Mo+peVpe
pk
M2peVo= Mpe1 M<peVpk
VoM2.(8c)
peVoVo+MpeVpk1 Mpe≥
VpkOntheotherhand,supposingthatthecircuitisideal,allthe
inputpowerPinwill nallydissipateontheload,i.e.,Pin=Po.UtilizingthecalculationofPinin(6c),theduty-cycledcanbesolvedas
√
d=2PofsL2
M.(8d)
peVpkEquation(8c)showsthattheDCMrestrictiondDCMdependsonMpeandtheline-andload-conditionsVpkandVo,itsvari-ationcanbeillustratedasFig.6(b).ItisseenthatthemaximalboundarydutycycleislimitedatdDCM=MpewheninputVpkislowandoutputVoishigh.Therefore,althoughasmallMpeleadstoalowdc-linkvoltageandhighinputPF,itresultsinasevererDCMrestrictionanddegradesthestep-downfeature.Forexample,ifPF=0.99isdesired,dDCM=Mpe=0.22mustbeselected,asshowninFig.6(b)(seethedashedregion).Asaresult,theactualdutycyclemustbelowerthan0.22evenwheninputVpkislowandoutputVoishigh.Referto(8d),ei-therPo,fs,orL2needstobedecreased,whichlimitstheratingpower,increasesthesizeofinductors,orincreasesthecurrentstressofthecomponents.Therefore,theselectionofMpemustbetradedoffduringthedesignprocess.
3)VoltageandCurrentStressesoftheSemiconductors:Ac-cordingtotheoperationalmodes,thevoltagestressesareeasytoobtain(seeTableI)andthus,wouldnotbeexplainedhere.However,thermscurrentsofthesedevicesarealittlebitcom-plicated.Here,thecurrentstressonthesingleswitchistakenasexample.First,thermscurrentofthesingleswitchwithinoneswitchingperiodcanbeexpressedas
iM
s rms Ts=
peVpkd3
L.(9a)2fs3Thermscurrentwithinhalfline-cycleperiodcanfurtherbe
obtainedas
I1 πM s rms=peVd3π is rms 2θ=pk0TsdL.(9b)2fs3Theresultsof(9a)and(9b)aretotallythesamebecausethe
singleswitchonlyneedstohandlethecurrentofthedc–dccell,andisnotaffectedbytheinputvoltagevariation.Withthesim-ilarmanners,IDa rms,ID1 rms,andID2 rms(thermscurrents owingthroughDaandthetwofreewheelingdiodesD1andD2)canalsobesolved,asgiveninTableI.Itisinterestingto ndthat,alltheseexpressionscanbeexpressedinsuchformsthatincludetheIs rmsterm.Physically,thisisbecausethesin-gleswitchSissharedbybothcells,therefore,current owing
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TABLEI
VOLTAGEANDCURRENTSTRESSOFTHEMAINS
EMICONDUCTORS
TABLEII
LOOK-UPTABLEFORTHERAPIDD
ESIGN
TABLEIII
SPECIFICATIONOFTHEP
ROTOTYPE
throughShasthenaturalrelationstothose owingthroughothercomponents.C.Summarization
ForatransformerlessS4converter,theparameterssuchasinputPF,inductionratio,dc-linevoltage,andduty-cycleareconcernedfordesign,buttheyareusuallycouplingandcompli-cated;however,theaforementionedanalysisshowsthatthere-lationsoftheseparametersintheproposedS4converterbecomequitesimple,assummarizedinTableII.TaketheintermediatevariableMpeasabridge,therelationsofinputPF,Landγcanbedeterminedimmediately,andthepossiblemaximalboundaryduty-cycledDCMandthedc-linkvoltageVbcanalsobeknown.Inotherwords,oncetheinductionratioLisdetermined,allthePF,thevoltagestep-downfeature,andthedc-linkvoltagestresscanbeestimateddirectly,regardlessofload-andline-variations.Theseuniquefeaturesfacilitatethecircuitdesignalot.How-ever,itshouldbeemphasizedagainthatalthoughthesmallerMpeleadstothehigherPFandlowerdc-linkvoltage,italsoresultsinthenarrowerrangeofdutycyclefrom0todDCM=Mpe,whichdegradesthestep-downfeature,thisfactormustbecompromisedduringdesign.
IV.DESIGNEXAMPLEANDEXPERIMENTALRESULTSA.PrototypeDesign
Accordingtotheanalysis,adesignexampleisgiveninthissection.Thespeci cationsoftheprototypearegiveninTableIII.
ThedesignprocedureissimpleduetotheuniquefeaturesoftheproposedS4converter.
Step1:SincePF=0.98isexpected,theinductionratioL=
0.31canbeobtaineddirectlyfromTableII.
Step2:FromTableII,themaximaldc-linkvoltageVb=
133Vcanbecalculated.Therefore,a160-Velec-trolyticcapacitorwithlargecapacitycanbeselected.
Step3:AccordingtoTableII,thepossiblemaximaldDCM
=0.31canalsobeknown;ontheotherhand,sincefsandPoarealsoknown,theactualdutycycledcanalsobedesignedaccordingto(8d).AsshowninFig.7(a),ifL2=7or14μHischosen,thedcurvewillalwaysbebelowthedDCMcurveevenwhenVpkchangesfrom127to373V(correspondingtothermsvoltagechangesfrom90to264V).ItimpliesthattheDCMconditionissatis edintheentireinputrange.However,ifL2is21or28μH,partsofdcurvewillbehigherthandDCMcurve,whichgoesagainsttheDCMcondition.Therefore,L2=14μHischosenheretosatisfytheDCMconditions.L2=14μHalsoleadstoamaximaldutycycleunderlow-linecondition(approachingto0.3),thecurrentstressesofthedevicescouldbealleviated.
Step4:OnceL2isdetermined,L1canbecalculatedasL1=
L2/L=45μH
Step5:SinceL1andL2aredetermined,thermscurrentsof
themainsemiconductorscanbecalculatedaccordingtoTableI.AsshowninFig.7(b),themaximalvalues
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Fig.7.Parametercalculation:(a)duty-cycleselectionand(b)currentstress
calculation.
Fig.8.Prototype:(a)maincomponentselectionsand(b)photographof
prototype.
Fig.9.Experimentalwaveformswithinseveralswitchingperiod:(a)and(c)fullloadand90-Vrmsvoltageinput;(b)and(d)fullloadand264-Vrmsvoltageinput.
ofIs rms=5.35A,IDa rms=4.27A,andID1 rms=3.29AappearwhenVpkisminimal;whilethevalueofID2 rms=7.7Akeepsconstantintheentireoperationalrange.
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Fig.10.Experimentalwaveformswithinseveralline-cycleperiodinfullload:(a)90-Vrmsvoltageinput,(b)110-Vrmsvoltageinput,(c)220-Vrmsvoltageinput,and(d)264-Vrmsvoltageinput.Step6:Finally,themaximalvoltagesofthesecomponents
canalsobesolvedaccordingtoTableI,thecalcula-tionsshowthatSandDaneedtohandleapossiblepeakvoltage506V,D2needstohandlethe
dc-link
Fig.11.Experimentalwaveformswithinoneline-cycleperiodinfullload:(a)90-Vrmsvoltageinput,(b)110-Vrmsvoltageinput,(c)220-Vrmsvoltageinput,and(d)264-Vrmsvoltageinput.
voltage133V,andD1needstohandlethemaximalinputvoltage373V.
Accordingtothecalculation,thecomponentselectionandthephotographoftheprototypearegiveninFig.8.AsimplevoltagefeedbackloopbasedonUC3842isusedandasimplePI
CHENetal.:DESIGNANDIMPLEMENTATIONOFATRANSFORMERLESSSINGLE-STAGESINGLE-SWITCHDOUBLE-BUCKCONVERTER
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Fig.12.Measurementresults:(a)dc-linkvoltage,(b)dutycycle,(c)rmscurrent owingthroughS,(d)inputPF,(e)THD,and(f)ef ciency.
controllerisdesignedtoobtainthedesired19Voutputvoltage.Sincethispaperfocusesonthecircuitcharacteristicsanalysis,someadvancedspeci cations,suchastransientresponseandhold-uprequirement,arenotconsideredintheprototype.B.ExperimentalResults
ThewaveformsofiL1,iL2,Vgs,andVds(thegatinganddrain–sourcevoltageofthesingleswitchS)withinseveralswitchingperiodaregiveninFig.9.InFig.9(a),theoutputisfullloadandthelowest127-Vinputvoltage(i.e.,90Vrms)isapplied,thedutycycleismaximal,however,iL1andiL2stillworkintheDCM;inFig.9(b),theoutputisstillfullloadbutthehighest373-Vinputvoltage(i.e.,264Vrms)isapplied,thedutycyclebecomesminimalandthemaximalvoltagestressVds≈510Vappears.Andinthebothcases,therestrictioniL2>iL1isalwayssatis edwhenSisturnedON,whichensurestheconductionofDa.InFig.9(c)and(d),thewaveformsofiSandiL2arefurthergiven.ItisseenthatwhenSisturnedON,thecurrent owingthroughiSandiL2arethesame,itveri estheconclusionthatthesingleswitchSonlyneedstohandlethecurrentofthedc–dccell.
Thewaveformsofiin ave[i.e.,theinputcurrentthathasbeensmoothedbytheLC lter,seeFig.8(a)],VbandVowithinseveralline-cycleperiodsaregiveninFig.10.TheoutputisfullloadandfourtypicalcaseswhereVpk=127,155,311,and373V(i.e.,90,110,220,and264-Vrmsvoltage)aregiven.Itisseenthatinallcases,iin avehasbeenshapedassinusoidal-likeform,andthemaximalVb=135VappearsinVpk=373V;inallthecases,theoutputvoltageVohasbeenregulatedas
19V.Fig.11furthergivesthedetailedwaveformsofVeq,vin,andiin aveunderVpk=127,155,311,and373Vsituations.ItisclearlyseenthatwhenVpkincreases,Veqalsoincreases,buttheirratioMpealmostkeepsconstant,thereforeγ(thelengthofregionII)alsokeepsconstant.Accordingtothewaveforms,γ=4/5π=2.51(rad)ismeasuredinallconditions,whichwellmatchesthecalculationinTableII.
InFig.12(a),(b),and(c),themeasuredandcalculatedVb,d,andIs rmsinfullloadarecompared;theymatcheachotherwell.InFig.12(d),themeasuredinputPFsunderdifferentline-andload-conditionsarealsogiven.ThemaximalandminimalinputPFsare0.975and0.96,respectively.Thedeviationbe-tweenmeasuredresultsandthedesired0.98ismainlycausedbythenonidealfactorswhicharenotconsideredintheanalysis,suchastheresistancesoftheswitchandinductors,thevoltagedropsofthediodes,thevoltage uctuationsonthecapacitors,andtheimperfectsinusoidalinputvoltageobtainedinthelab.Thesefactorsbecomedominantwhentheinputcurrentislow,therefore,thePFslightlydecreaseswheneitherthelinevoltageincreasesortheloaddecreases.However,thedeviationbetweenthemeasurementanddesiredvalueislessthan1%innormalcondition(PF=0.974infullloadand220Vrmsinput),andlessthan2%evenintheworstcase.Suchaccuracyissatisfac-toryenoughtoensuretheTHDoftheinputcurrentcomplianttoIEC61000-3-2,ClassCstandardintheentireoperationalrange,asshowninFig.12(e).
Finally,theef ciencyoftheprototypeisgiveninFig.12(f).Itisseenthatthebetteref ciencyperformanceappearsinmediateloadandthenormal110and220Vconditions.Themaximalef ciencyis89%.SincetheproposedS4converterisactually
6670IEEETRANSACTIONSONPOWERELECTRONICS,VOL.29,NO.12,DECEMBER2014
anintegrationversionofthetwo-stagestructure,itsef ciencyisrelativelylowascomparedtothetypicalsinglebuckPFCsforlightingapplication(forexample,the12-W/22.5-V-tappedinductorbuckPFCin[2]providesanef ciencyof90.2%,the13-W/19.8-Vresonance-assistedbuckPFCin[2]providesanef ciencyof92.8%,andthe150-W/145-VbuckPFCin[9]providesanef ciencyupto96%).However,comparedtoothertransformerlessS4converters,the89%ef ciencyissatisfactory(forexample,thetransformerlessS4convertersin[33]–[38]havethesimilarpowerlevelfrom20to100W,andtheiref -ciencyare77%,80.5%,85%,89%,and89.5%,respectively).ThemainlossesoftheproposedS4convertercomefromthetwiceenergyprocessingbythePFCanddc–dccells,thecon-ductionlossoftheadditionaldiodeDa,andthehighrmscurrentintheDCM.
Theexperimentsalsoshowthat,toensuretheconstantinputPFfeatureandacceptablevoltageripples,bothCbandCoarerelativelylargesothatVoandVeqkeepalmostconstant,thisisoneofthemaindisadvantagesoftheproposedS4converter.Fortunately,thecapacitorswithlowratingvoltagebutlargecapacitance(forexample,1mF/160Vand1mF/35V,here)canbeutilizedduetothelowdclinkandoutputvoltage.Besides,theoutputground(Coground)intheproposedS4converteris oating.The oatinggroundoutputisallowedinthelightingapplicationsbecausetheirloads(forexample,theLEDs)aretotallystandalone[2],[31],[37],[38].However,the oatinggroundcontributesanadditionalcommon-mode(CM)noisesource,andtheCMnoisewillinjectintothegridthroughtherecti erdiodes.Nevertheless,thisproblemcanbesolvedbyinsertingaCMchokebetweenthegridandtherecti er,asthosein[8],[9],and[39].SincetheCMchokeissmallinsuchpowerlevel,itwillnotincreasethesizeandcostdistinctly.
V.CONCLUSION
ThispaperproposesatransformerlessS4converterintegrat-ingabuckPFCcellandabuckdc–dccellinanovelway.Theproposedintegrationleadstosomeuniqueline-andload-independentfeatures,whichfacilitatethecircuitdesign.Ac-cordingtotheanalysis,thefollowingconclusionsareobtained:1)duetotheintegrationoftwobuckcells,ahighstep-downfea-tureisobtained.Inlow-lineandfull-loadconditions,thedutycycleoftheprototypeisupto0.3,andinhigh-lineconditionisstill0.1;2)thebuckPFCcellleadstoalowdc-linkcapacitorvoltagenothigherthan160V,thereforeanelectrolyticcapacitorwithlow-voltageratingbutlargecapacitycanbeused,3)thesin-gleswitchonlyhandlesthecurrentofthedc–dccell,thecurrentstressislow,4)thelengthofregionIIkeepsconstant(γ=4/5π)regardlessofline-andload-conditionsvariation;theinputPFisveryclosedtothedesiredvalue,andtheinputharmoniccurrentsarecompatiblewiththeIEC61000-3-2,ClassCstandardintheentireoperationalrange.Duetothesebene ts,theproposedS4convertercanbetreatedasacost-ef cientcandidateforthelow-power,nonisolated,andstandalone-loadapplicationswhereahighinputPFandastableoutputarerequired.
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YuChen(S’09–M’11)receivedtheB.E.andPh.D.degreesinelectricalandelectronicengineeringfromtheHuazhongUniversityofScienceandTechnology,Wuhan,China,in2006and2011,respectively.
FromMarch2008toMarch2009,hewasanIn-terninGEGlobalResearchCenter,Shanghai,China.InSeptember2011,hejoinedtheHuazhongUni-versityofScienceandTechnologyasaLecturer.Hisresearchinterestsincludethepowerelectronicconvertertopologies,soft-switchingtechniques,con-vertermodeling,thefaultdiagnosistechniques,and
thewindenergypower-conversion
system.
ZhihaoZhongwasborninGuangdongProvince,China,in1989.HereceivedtheB.S.degreeinelec-tricalengineeringfromtheUniversityofElectronicScienceandTechnologyofChina,Sichuan,China,in2012.HeiscurrentlyworkingtowardtheM.S.degreeinelectricalengineeringintheHuazhongUniversityofScienceandTechnology,Wuhan,China.
Hiscurrentresearchinterestsincludepowerelec-tronicssystemintegrationandhigh-ef ciencycon-
verters.
YongKangreceivedtheB.E.,M.E,andPh.D.de-greesfromtheHuazhongUniversityofScienceandTechnology,WuhanChina,in1988,1991,and1994,respectively.
In1994,hejoinedtheHuazhongUniversityofScienceandTechnologyasaLecturerandwaspro-motedtoanAssociateProfessor,in1996,andtoaFullProfessorin1998.HeiscurrentlytheHeadoftheCollegeofElectricalandElectronicEngineering,HuazhongUniversityofScienceandTechnology.Heistheauthorofmorethan60technicalpapers.Hisre-searchinterestsincludepowerelectronicconverter,acdrivers,electromagneticcompatibility,andtheirdigitalcontroltechniques.